Duplex switch with leakage compensation



Sept. 7, 1948. C, F, P RQSEl 2,448,623

DUPLEX SWITCH WITH LEAKAGE CMPENSATION /NVE/von SE C. F. P. ROSE DUPLEX swITcH wITH LEAKAGE COMPENSATION Sept. 7, 1948.

2 Sheets-Shes?. 2

Filed Feb. 15, 1945 .ul .ul c..

TJII u T ATTURNE'V Patented Sept. 7, 1948 DUPLEX SWITCH WITH LEAKAGE COMPENSATION Charles F. P. Rose, Asbury Park, N. J., assigner to Bell Telephone Laboratories, Incorporated, New York, N. Y., a corporation -of New York Application February 15, 1945 Serial No. 578,073

`11 Claims. l

The invention relates to a two-Way signal transmission system, and particularly to coupling and switching arrangements for use at a terminal 'ofsucha system to enable proper two-'way operation'where the signal transmitting and freceiving circuits are coupled to a two-Way signal transmission medium through a common transmission devicesuch as an antenna.

Although 'the coupling and switching arrangements ofthe invention are applicable -to any wire or -radio'si'gnal transmission system of the duplex type, they'are particularly adapted for and Will be described as 'applied to an object-locating system of thepulse .reflection type, for example, `one employing ultra-high frequency or radio Waves, commonly 'called a radar system. In the usual radar system, very short pulses of high 'frequency signal energy are generated and radiated at frequent intervals through an antenna at an observation point into a surrounding air wave transmission medium; return pulses, which may be termed radio echoes, reflected from objects to be located in the transmission medium are-picked upby the same antenna and are detected in a-n associated tuned signal receiver; and the detected pulses are compared on a time basis in a suitable `measuring or 'indicating circuit with `the outgoing signal pulses so as to provide a measure ofthe distances `to the objects causing the echoes.

rvUsually such systems employ extremely sensi- `tive apparatus, such as tube or crystal'detectors, in theirreceiving circuits, which may be destroyed er have their operation characteristicsI substantially impaired if subjected to very high voltages such as would necessarily be used yfor theoutgoingfsignal `Wave energy. To provide proper durplexmceration and prevent injury tothe `sensitive receiving apparatus, signal controlled switching devices have been used with such systems ,to insert.asuitable loss in the input to the receiver during signal transmitting intervals and `to 1remove :that loss during signal receiving intervals. in one such system of the prior-art disclosed `in the 'copending 'United States patent application cfr.. L, Samuel, Serial No. 474,122., vfiled-January '(30, 1943, a coaxial vor Wave guide line is employed .for connecting the signal transmitter or outgoing signal pulse generator to the antenna or other `common Ysignal ktransmitting .and receiving device, and the signal controlled switching vdeviceenlployed for the above purpose Vcom- .prises a hollovv'chamber or cavity with .Wallsrof 'conductive finaterial, suitably `dirnensioned .and .designed so` as lto be resonant tothe frequ'ency ofthe ncomingand outgoingsignals, with agaseous discharge tube connected across it, .coupling the input :of the signal receiver to the main line at a suitably Alocated branching point. The gas tube is adapted to discharge in response to the high resonant voltage built up across it'by the portions Aof the outgoing signal pulse energy entering the resonantchamber during signal transmitting intervals, so as 4to provide alow impedance shunt across the chamber operatingito detune the latter and thus to appreciably reduce the amount'of this signaling energy'reaching the signal receiver, and to remain in the undiseharged condition to maintain .the resonant chamber tuned and thus the transmissioneile ciency of the receiving .circuit high for theV relatively low voltage incoming signal ipullse energy entering the resonant vchamber during signal receiving intervals.

An object of Ythe invention is to improve a couplins and switching device ofthe above-described type, particularly from the standpoint of reducing vthe amount of high power leakage lthrough the device Ato the local receiver during 4signal transmitting intervals.

A more specific obj ectisto so Areduce '-h-igh power leakage through `a signal controlled switching device `of the resonant chamber-gas discharge tube type in a rradar system or terminal of :a duplex signal Wave transmission system, as to prevent `injury `or substantial impairment of 'oper-v ation of associated sensitive signal .receiving apparatus, such yas Vcrystal detectors, and Without adversely affecting its operation for low `power signal inputs.

These objects are attained in accordance with the invention by the addition `to a-system ofthe above-described type, of an arrangement for -abstracting sample energy portions of the signal waves or pulses V'transmitted over the main fline connecting the outgoing signal lwave generator to fthe Vantenna or ,other common transmitting and receiving device; for transmitting thesesample signal energyportions over an auxiliary transmission path tovvards the output Aor ,the ,resonant `,chamber .of the transmit-receive ,switchingclevice and .for .there vcombining the Signal output 4of the latter .path .with the ,signal ,output .of the resonant 4chamber in proper .phase Vand magnitude so as :to effectively cancel the lhigh power `.leakage :through the device; rand yformal;- ing the attenuation of the @auxiliary path equal .to ithat ,afforded by Vthe :resonant chamber when itiis `tletll-riefi through Ithe function ofptheassoci- 'atedrshuntinggasuischarge device, so astovavoil to cancel the high power signal leakage through the other chamber normally resonant to the sig nal frequency when the latter is detuned by the discharge of the associated discharge device in response to the portion of high power outgoing signal energy entering that chamber during sigf nal transmitting intervals, The normally detuned condition of the cancellation chamber is utilized to prevent it from causing suppression of the low level incoming signal energy transmitted through the other normally tuned chamber to the local receiver during signal receiving intervals.

The various objects and features of the inven- .tion will be better understood from the following detailed description when read in conjunction With the accompanying drawings in which:

Each of Figs. 1 to 3, inclusive, shows schematically a portion of -a radar system employing coupling and switching arrangements shown partly in section, embodying the invention, the arrangements of these figures differing only in structural details;

Figs. 4 and 5 show a front elevation View and a sectional view, respectively, of a switch assembly illustrating one practical embodiment of the invention; and

Fig. 6 shows a perspective view, partly broken away, of a portion of the coupling and switching 'arrangement of Figs. 4 and 5, illustrating diagrammatically the means employed for providing the required 180-degree yphase diiference between the outputs of the two resonant chambers.

In the radar systems `of Figs. l and 2, a main line L1 comp-rising a section of coaxial line having inner and outer concentric conductors I and 2, respectively, vconnects the signal transmitter T to the common transmitting and receiving antenna A. The signal transmitter T may be of the magnetron type, adapted to generate recurring electric signal pulses of ultra-high frequency, such as disclosed, for example, in the United States patent of A. L. Samuel 2,063,342, issued December 8, 1936. A longitudinal slot 3 is cut in the outer conductor 2 of the main coaxial line L1 at -a suitably located branching point B intermediate the transmitter T and the antenna A. A sector of pipe l having a small aperture or window cut in it at a mid-point is adapted to slide over the portion of the outer conducto-r 2 of line L1, containing the longitudinal slot 3.

A section of hollow metal wave guide 5, which may be of rectangular or circular cross-section, is mounted on the face of the pipe sector 4 at a point adjacent the aperture therein, so that its longitudinal axis is yperpendicular to the longitudinal axis of the main line L1. The Wave guide section 5 is closed at its far end with a piston or plunger The interior of the wave guide section 5 is connected at its near end through a small window or iris 7 formed by the intermediate aperture in the pipe sector 4 and the adjacent portion of the longitudinal slot 3 4 in the outer conductor 2 of the coaxial line L1, with the interior of that line.

The interior portion of the wave guide 5 be tween the iris 1 and the piston 6 forms a hollow chamber or cavity RC, the dimensions of this chamber and the size of the iris 1 being selected so that the chamber is resonant at the frequency of the outgoing signals generated by the signal transmitter T and of the incoming signals received yover the line L1 from the antenna A. The tuning of the resonant chamber RC may be changed within given limits by adjustment of the the position of the plunger 6 in the wave guide 5 so as to change the effective length of the chainber, thus adapting it for changes in the frequency of the incoming and outgoing signals. A metal loop 9 in the chamber RC near its far end connects through apertures in one side cf the wave guide 5 to the inner and outer conductors of a second coaxial line L2 which extends through to a suitable signal receiver R. The loop 9 provides coupling at the frequency to which the chamber RC is tuned, for transmission to the signal receiver. A Ipair of spark-gap electrodes li) and Il are connected to opposite sides of the resonant chamber RC at a Ihigh impedance point (near the electrical :center o-f the chamber), to provide a discharge gap between them adapted to be broken down to short-circuit the chamber when a sufficiently high resonant voltage is built up across the gap. As indicated diagrammatically, the electrodes it! and Il may be enclosed in a suit-able vessel or tube 8 containing an atmosphere of gas at low pressure, so that the spark-gap may be easily broken down by the high voltages which would necessarily be used for the outgoing signals in such a system.

In the usual operation of the system of Figs. 1 and 2 as described, the energy of the high frequency pulses from the transmitting pulse generator T during signal transmitting periods flows over the main coaxial line L1 toward the antenna A. Part of that wave energy will be transmitted to and radiated by the antenna A to the associated wave transmission medium, and another 'portion will be diverted from the line L1 at the branching point B through the iris coupling 1 into the input of the resonant chamber RC and will build up across the gap between the spark-gap electrodes i@ and Il a sufliciently high voltage to cause an arc discharge in the gap between those electrodes. The effect of this is to produce a low impedance shunt across the chamber RCl at a maximum impedance point and thus a lower apparent impedance across the input of that chamber. The effective short-circuit thus produced at the coupling iris 'l will detune the chamber RC so as to substantially reduce the amount of pulse energy of the resonant frequency tnansmitted through the chamber and thus the amount of high power signal energy passing to the signal receiver R by way of the output loop 9 and associated coaxial line L2. The relatively low resonant voltage of the portion of each incoming signal pulse received during signal receiving periods over the coaxial line L1 from the antenna A, which is diverted into the input of the resonant chamber RC through the coupling iris l, will be insumcient to cause the sparkgap between the electrodes Iii and Il to break down, so that there will be no short-circuit produced across the resonant chamber RC. That chamber, therefore, will be maintained tuned to the signal frequency so as to allow transmission of the received signal pulses through the resoandere nant chamber and `the coaxial .line La to the signal receiver R with Icomparatively little loss. By V proper adjustment ofthe pipe sector f4 along the outer .conductor 2 of .the coaxial :line L1, the lengthv oi linewbetween the .signal transmitter T and the input `iris`1 of 'the .resonant chamber `B (branching point B), may be made such that substantially all of thev received :incoming signal energy may .be diverted Afrom the vcoaxial line L1 into Vthe resonant .chamber RC.

l By mounting 'theoutput loop 9 on the face Vof the tuning plunger (i, as indicated, and rotating this loop so that itsfplaneis at an optimum angular position. with respect .to theV face of the plunger, the amount of high power leakage through the chamber during signal transmitting periods may vbe made .independent of the tuning frequency used over a given Vfrequency range.

In systems of the above-.describedtype in which crystal detectors are employed in the vsignal receiver, the high power leakage through the resonant chamber of such .a transmit-receiveswitch may be high enough to destroy or substantially impair the 4operation of l.the crystal detectors. This is prevented in accordance with the .present invention `by the addition of suitable auxiliary arrangements for abstracting energy samples of the outgoing signals applied to the input of the resonant chamber during signal transmitting intervals, for transmitting these samples over an auxiliary transmission path of suitable characteristics towards the output of thereson'ant chamber and for there combining the signal output of the auxiliary path with the signal output of that chamber in proper phase and magnitude to effectively cancel out the high power leakage component through the chamber during signal transmitting intervals.

In one arrangement for accomplishing this. illustrated schematicallyin Fig. 1 the cancellation voltage is introduced through a length of flexible coaxial cable La which .connects a voltage probe l2 extending into the interior of the main coaxial lineLi at a suitable :distance longitudinally from the branching point B, to `a T 'junction with a lead from the output loop El of the resonant chamber RC. Preferably, the end of the flexible coaxial cable La is capacitively coupled with the output lead at this point, as indicated, so as to segregate the cancellation path from the output pat-h of the resonant chamber RC .and to provide a desired amount of insertion loss to the low level incoming signals and to prevent the introduction of additional low level loss in the latter path. This capacity. coupling is also used to supply a portion of the necessary attenuation in the cancellation path required so as lto prevent the latter from causing cancellation of the low level incoming signals diverted from the main line L1 into the resonant chamber RC .during signal receiving intervals, when vthat chamber is tuned to transmit these signals efficiently. The total attenuation provided by the cancellation path including cable La and its associated couplings should be equal to the attenuation afforded by the resonant chamber RC when it is detuned by a breakdown of the associated-discharge gap between electrodes Ill and il in response to the high level outgoing signals. The necessary 18o-degree lphase difference between the signaloutput of theA cancellation cable La and the signal output of the resonant chamber RC maybe obtained by the provision of a termination M at the input end of that cable adapted for slidable vmovement on the outer conductor 2 of the main coaxial line L1 to provides. given amount of longitudinal movement in` either direction from a given point of the probe l2` within the line L1, sor'as to enable its positioning at :'a properdistance from the branching point B. 'Tests of a radar arrangement, similar to that illustrated in Fig. 1, in combination with the cancellation arrangement shown in that gure indicated that during signal transmitting intervals the :reduction in high power leakage through the :resonant chamber at a frequency of 2745 megacycles was in the order of 16 decibels.

Cancellation of the -high power leakage by using a cancellation `path excited from a point removed longitudinally along the main coaxial line Lrrequires that the point of connection B of the resonant chamber RC of the transmit-receive switch to that line -be adjusted along the line for the voptimum operating point. The cancellation scheme illustrated in Fig. 2 avoids this requirement by the selection of a. pick-up point for the cancellation voltage adjacent to and symmetriu cally located with respect to the center point of the input iris l for the resonant chamber RC. Instead Aof employing a probe pick-up as illustrated in 1, in the arrangement of Fig. 2 a pick-up loop `I5 is provided 'for coupling at this point, so that the cancellation path L3 and the resonant chamber RC are current excited from a common point'on the line L1'. When employing such a loop, the `degree of cancellation is essentially independent of the position of the resonant chamber R'C `along the main line L1. Also, in the cancellation arrangement of Fig. 2, the required phase vand magnitude of the cancellation voltage is respectively accomplished by proper orienta-- tion of the input loop l5 and adjustment of the eiiective length of the cancellation path by means of a telescoping section I6 of the coaxial cable employed for that path.

.The modified arrangement of the invention illustrated in Fig. 3 differs from that of Fig. 2 merely fin that the mechanical design of the resonant chamber RC has been simplied by the elimination `of vthe tuning plunger 5 and the substitution of the metal tuning screws or plugs Il and I8 extending through properly located opposite points in the side walls of the chamber, the tuning of the chamber depending upon the degree oi penetration of these screws. Thus, a d-ouble mode, plug-tuned resonant chamber adapted to transmit .a band of frequencies is obtained.

Figs. 4 to 6 show various views of a portion of a `radar system employing a resonant chambergas discharge tube type of transmit-receive switch, and an associated high power leakage cancellati-on arrangement in accordance with the invention `which has been found to be particularly eih'cient. The transmit-receive switch includes a sector of .pipe 4 having two centrally located apertures |9a and |917, adapted to slide along the portion containing longitudinal slot 3 of the outer concentric conductor 2 of the main coaxial line L1 which connects the signal transmitter or pulse .generator T to. the common transmitting and receivingantenna. A.

Mounted on the pipe sector 4 symmetrically with respect to its two apertures lila `and I9b is a metal box or housing 20 containing adjacent to each other two identical hollow metal-walled chambers lor cavities, RC and CC, of rectangular cross-section with their longitudinal axes perpendicular to thelongitudinal axis of the main coaxial line L1. The chambers RC and CC are of the; general double mode plug-tuned type illustrated in Fig. 3. each chamber including two tuning plugs 2| and 22 extending through the side walls of the chamber at respectively opposite points, which are utilized for adjusting' the resonant frequency of the chamber to the desired value; an individual gas discharge tube 23 the dis-charge path of which is connected in shunt with the chamber at a high impedance point; individual input irises provided by the apertures lila and lSb, respectively in the pipe sector 4, which are so located as to'respectively connect the interior of the chamber' RC and the interior of chamber CC to the interior of the main coaxial line Li through the longitudinal slot 3 in its outer conductor 2; and an individual output loop 23, 21 in the end of each chamber opposite the input iris. The auxiliary box-like projections 28, 29 attached to opposite outer walls of the main housing serve to form a protective housing for the gas tubes 23 and may be unscrewed to allow the tubes to be removed or replaced.

The gas-filled tube 23 may be of any suitable type. The particular gas-filled discharge tube illustrated consists of an outer glass vessel enclosing an atmosphere of gas at'low pressure, a pair of main electrodes 30 and 3| within the vessel, having axially aligned frusto-conical portions mounted with their smaller ends in juxtaposition and defining a spark-gap, and an auxiliary electrode 32, termed an ignitor or keep alive'electrode, formed by a rod extending partly within the frusto-conical portionof one of the main electrodes, During operation of the tube 23, the auxiliary electrode 32 is maintained at a fixed negative potential with respect to the main electrodes 38 and 3l by an associated power source (not shown) whereby a glow discharge is maintained between the auxiliary electrode and the adjacent frusto-conical portion, this discharge being substantially confined to the region outside of the high frequency eld region between `the main electrodes. The function of this glow discharge is to reduce the time or voltage required for ionization in the tube. This in turn reduces the leakage power through the chamber RC or CC at the initiation of the iring of the associated gas tube. In each chamber RC and CC, the main electrodes 33 and 3|' are connected to opposite chamber walls at a high impedance point (electrical center) of the chamber, effectively in shunt with the input iris couplings I9a and leb, respectively. `The tube constants are selected so that the maximum voltage of the resonant frequency built up across the associated gas tube 23 by the energy of each outgoing high power signal pulse diverted into the .chamber through its input iris will cause the gas in the tube to break down and a discharge to take place across its spark-gap so as to provide a low impedance shunt across that chamber. With the tube constants so selected, the relatively low voltage of the portion of each incoming signal pulse diverted into the chamber through its input iris will be ineffective to cause discharge of the tube 23, and the chambers RC and CC will be maintained in their normal tuned or untuned conditions respectively, determined by the adjustment of their tuning plugs 2l, 22, with respect to the signal frequency so as to allow or prevent, respectively, eiicient transmission of the applied signal pulses to the individual output loop 26 or '21 of the resonant chamber.

The individual output coupling loops 2G and 2l of the resonant chambers RC and CC, respectively having respectively reversed wiring arrangements illustrated in Fig. 6 to be described later, are connected through a T juncton 33 to the inner and outer conductors of va section of coaxial line L4 including the quarter-Wavelength line 34 operating as an impedance matching transformer. The section of coaxial line L4 feeds into the signal receiver R indicated as being of the superheterodyne or double detection type. In that receiver, the incoming signal energy received over the line L4 is combined in the rst detector stage 35 comprising a crystal converter, with beating oscillations of suitable frequency supplied over a branching coaxial line Ls coupled to the coaxial line L4 in the input of the detector 35 by the adjustable telescopic section 36, to beat the signals down to an intermediate frequency which may be amplified in an intermediate frequency amplifier, detected in a second detector stage and supplied to a suitable signal recorder or signal receiver as in the usual superheterodyne receiver.

One of the chambers RC and CC with its associated shunting gasvdischarge tube 23 is utilized to perform the function provided by the path L3 in the system of Fig. 3, thatvis, to provide effective cancellation of the high power leakage through the other chamber during signal transmitting intervals while allowing the relatively low power incoming signal energy to be transmitted through the latter chamber to the signal receiver during signal receiving intervals with little loss. This is accomplished by the provision of means for making the wave outputs of the two chambers RC and CC equal during signal transmitting intervals when equal portions of the outgoing signal energy are applied to the inputs of these chambers from the common branching point on the main coaxial line L1 and for combining these equal outputs in phase opposition so as to effectively prevent any energy from being transmitted to the receiver R during these intervals; and by making the attenuation of one of the chambers, say, CC, utilized for the cancellation chamber during signal transmitting intervals of a value such that during signal receiving intervals when equal portions of the low level incoming signal power are applied to the two chambers from the common branching point on the main line, the signal output from the cancellation chamber will be substantially zero and thus there will be no cancellation of any of the low power signal energy transmitted through the other resonant chamber RC which remains tuned to the signal frequency. The latter is attained by proper adjustment of the tuning plugs 2l, 22 of the cancellation chamber CC so that it is normally detuned from the signal frequency.

Cancellation of the high power leakage is accomplished when the tuning plugs of the cancellation chamber are adjusted to give the proper current amplitude in the cancellation loop. The proper phase relation of the currents in the two output loops for cancellation is obtained by complementary orientation of the output loops in the two chambers. As seen in the wiring schematic of Fig. 6, to accomplish the latter result, the conductor forming the output loop 26 in the chamber RC extends from the T junction point 33 through a hole near one chamber wall into chamber RC in which it is bent back on itself and fastened to a ground point 31 on the chamber wall with a developed lead length of onequarter wavelength, and the conductor forming the output loop 2l in the resonant cavity CC extends from the junction T 33 through a hole in one wall of the chamber CC into that chamannesse-1 impedance at the juncti'on'ffrom-one circuit"'to":15

the other.Y

A dummy tube, su'ch as acohtinudusb'pst: between the chamber walls having 'an' ei''ectivefimpedance equal to that 'cf the gas tube@usedA the main resonant vchamber,v in' the `u hdifschargjfgcl conditioncould be used in"theeancellati'niicliam` ber ofthe arrangement ofFigsx/ito; in the'pl-a'e" of the gas tube in thaty chamber; at'af positicn' corresponding'to thatv of the active tube infthe other resonant chamber, but-it has been/"fo that the use of active gasy tubes' ini both'charn-j bers gave better cancellationofthe-'highpowerL leakage components particularly wl-i'enfalreepfalive voltage is applied to bothtubes," whichj may beattrihuted tothe facttha-t'thegasiieak; 3

age component as well as thedirect'rlealagecomi ponent is reduced. Furthermore# the amount-fof" spike at the leading edgeOttheW-pulse` could' also be reduced with the twotubearrangerren Tests of a radar systerrremplyingfacresen chamber gas-discharge'4 tube' transmit-rece switching arrangement' of the twincha-rnb erjl efillustrated in Figs. 4 to6,'4 incombinatiohfwith'a" coaxial line delivering about'BOO' kilowatts-o In other" 5 power to the common 4transmitting'and dreceiv` 40 ing antennashow that with,"aolditich'oilapronL erly adjusted cancellation' pathJ ofthejlattfer aitrangement a. reduction of theihisht'povverdeaktl age through theswitching arrargementv signal transmitting intervals in the' about tldecibels' can be obtained.- h

use of this cancellationvschernel; itlwasf'drm"l the crystal detectors used intheisigalfreceiver" would be substantially-in'ipairedbyJ the Lhi'gh'pt'iw-` er leakage.

Various mcdications of? thearrangementsjfofj the invention illustrated anddescrileedwhich are within the spirit andscope'of thejinventior'i will occur to persons skilledintheart.`4

What is claimed is:A

1. In combinations, common linelfor'rtr'ansf" mitting at diierent timeshigh power alterhatirig'L current signals and vrelatively 4low powerbalte nating current' signals,v a signal receiver;A afoou pling device normally resonant' tothefre'quen of said low power and highpowersignalslco necting said receiver to'said line, control means connected tosaid line through a portionovffsaif" coupling device, operatively responsive jto' 'ther'err ergy of the high power signalsappliedthereto" 65 through said deviceV todetune the latter sortlf'rat" the amount of high power'signaling' energyreafc'h'f ing said receiver is appreciably reducedsaid trol means being unresponsive to the-rela tive low power signals appliedtheretdthro gh device so that said* device" is maintairim to transmit said low powerVV signalseiciently tof*` said receiver and auxiliary means 'to'providej further protection of said"rf e`ce`iw'/er fro'rrrsaid" 10 tinuously abstract sample energyfportioris`of"the transmitted signals from said line and means to 'combine the high power signarconipohen'ts only of th'el abstracted sampleenergyportiohs with thesi'gnal output of said 'couplin'gde'vice in such' manner 'as to substantially suppress the' 'high powersignai leakage through said coupling devicewhen' the latter is detuned byoperation of' theassociatedcohtrol device' in response'to'ap-J` lied high' power signals. l

2. The" combination of 'claim '1, in Vwhich 'sai'd auxiliary means comprises a signal'by-'passingA circuit lconnecting the input and output offsaid coupling device,'means in said'bypassing-circuit for making the amplitude and phase ofthe power signal output thereof such that it effec; tively balances out the'high powerfsigrial leakage through said coupling device when the'1 `latter`is detuned, andother'me'ansto make the vattenuation ofrsaid by-passingcircuit ly large to prevent transmission of any substanf tial amount of the low powerv signaling energy` therethrough to the output of said coupling `device.

3.'Tl`1e combination of claim 1,- irr which said auxiliary means comprises an additinal translmission path connecting said line to l the 'output of said coupling device! the effective length o f. sa i d l path and its poling with respect to the inputv and 0 output rof said coupling device being such 1that When said coupling device is detuned by Qperation of said control means in responseto1 high power signal energy applied from said line; theamplitude and'v phase ofthe Vhigh powersignal energy output of said additional transmission path is such that the latter effectivelycancels out-the high power signal'leakage throughfsaid coupling `device. 4. The'combination of vclaim 1, in which sai d. coupling device comprises a hollow wave guide resonant chamber coupling said receiver lt said line at a given point and adjustable tuningheans therefor', said energy-responsive control niears comprises a gas discharge device connect'edac'ro'ss `said chamber, adapted to discharge'to provideaa" low impedance detuning shunt ther'eacross response to the applied voltage produced bythe highpower signal energy entering'said chanibe from lsaid une, and to remain undischargedt 0 maintain thecharn'ber tuned in response ,tothe relatively'lower applied' voltage produced'by',` low powerl signal energy entering said chaniber from" said line, said' auxiliarymeans' comprises a second couplingdeviceincludinga second*reso^' high power signals comprising vmeans? `to: co'r'il 75 vsothat` infthe latter conditionthe-'high 'powerAll 55A nant"charnber identical with the first 'resonant' charge device land adjustable tuning meansj: re-AV spectively,` identical with the detuning"gas" di f charge device and the tuning means'` associated" withsaid first chamber, coupling 's aidsigiiahre-E ceiver'to'said line atsaid given point, thetunirig means associated `with Asaid'rst andsecond-frese"-A nant` 'chambers being respectively adjustedj so that' in v the absence of applied high power sigrralsjA said rst chamber is ltuned to thej'frequencyof said signals and said second chamber is: de t'un'ed'* from lthatA frequency, and so that'iw h'eljfhigh power *signals* are applied to the;inputs'jofbthlf chambers ythe output voltage-#of s aifd second 'j'- chamber is equal to that of saidfrlrst ich meerj when the latter is detuned bythe''con s eqiient-l discharge of the associated `discharge"devi nd` the outputs' of the twochambers withfrespectf the inputof "said receiver are respeetively pha chamber, and an associated detuninggascis-'f 1 l leakage components through said rst chamber are effectively balanced out.

5. In combination, a line transmitting high power and low power alternating current signals at different times, a signal receiver, a branch transmission circuit connecting said receiver to said line, including a hollow wave guide chamber resonant to the frequency of said high power and low power signals, a discharge device connected across said chamber, adapted to discharge in response to the applied high voltage of the high power signals entering said chamber from said line to produce a low impedance shunt across the chamber thereby detuning the latter so as to appreciably reduce the high power signal input to said receiver and adapted to remain undischarged in response to the relatively lower applied voltage of the low power signals entering the chamber to maintain the tuning of the latter so that it transmits the latter signals efficiently to said receiver,

and means to substantially suppress the high power signal leakage through said chamber when it is detuned comprising a signal by-pass circuit connected around said chamber, means in said by-pass circuit for making the amplitude and phase of the high power signal output thereof when said chamber is detuned by applied high power signals, respectively equal and opposite to that of said chamber, and other means to prevent suppression by said by-pass circuit of the low power signals transmitted through said chamber.

6. The combination of claim 5, in which said other means comprises means for making the attenuation of said by-pass circuit equal to that of said chamber when it is detuned by the discharge of said discharge device.

7. In combination, a source of low power and high power electric signals at respectively different times, a signal receiver, a hollow wave guide chamber resonant to the frequency of said low and high power signals, having its input electrically coupled to said source and its output electrica-lly coupled to said receiver, a discharge device connected across said chamber, adapted to discharge in response to the high voltage applied thereto by the high power signals entering said chamber thereby providing a low impedance shunt thereacross which detunes the chamber so as to reduce the amount of high power signal energy supplied to said receiver, and adapted to lremain in the undischarged condition in response to the relatively lower voltage applied thereto by the low power signals entering said chamber thereby maintaining the chamber tuned to transmit the latter signals eiciently to said receiver, auxiliary means for abstracting from said source and separately supplying to the output of said chamber energy samples of the high power signals applied to the input of said chamber, in proper magnitude and phase with respect to the signal output thereof as to effectively cancel the high power leakage through said chamber, and other means to prevent said auxiliary means from causing cancellation of low power signals transmitted through said chamber during low power signal transmitting intervals.

8. The combination of claim '1, in which said auxiliary means comprises a circuit for by-passing a portion of the energy of the high power signals from said source around said chamber to the output thereof, the effective length of said by-passing circuit being selected and the poling thereof with respect to said chamber being adjusted to provide the required magnitude and phase of the by-passed signal components at the output of said chamber for high power leakagecancellation, and said other means comprises means for making the attenuation of said bypassing circuit equal to that of said chamber when it is detuned by the discharge of said discharge device.

9. The combination of claim 7, in which said source comprises a main line having a tubular outer conductor, and means to transmit low and high power alternating current signals at respectively different times in opposite directions over said line, said resonant chamber includes metal tuning plugs adapted for insertion therein to different distances to adjust the tuning of the chamber over a desired frequency range, said chamber being electrically coupled at its input to said main line at a given intermediate point through an iris opening in its outer tubular conductor and being electrically coupled at its output to said signal receiver through an output pick-up -loop within said chamber, said auxiliary means comprises a second resonant chamber identical with the first chamber also coupled at its input to said main line at said intermediate point through said iris opening in said outer tubular conductor, and being connected at its .output through an individual output loop to the output loop of the iirst resonant chamber through a T junction, the individual tuning plugs of said second resonant chamber being adjusted to give said proper magnitude of the high power energy samples in its output loop, and the output loops of the two chambers being oriented in complementary relation so as to provide said proper phase of the high power energy samples in the output loop of said second chamber for cancellation of high power leakage through the first resonant chamber, said other means comprising an adjustment of the tuning plugs of said second chamber so that the latter is normally detuned from the frequency of said low power signals.

10. In combination with a duplex signal transmission system including at a terminal thereof a common line having an outer tubular conductor, for transmitting outgoing alternating current signals oi high power in one direction thereover and incoming alternating current signals of the same frequency and of relatively low power in the opposite direction thereover and a signal receiver for said incoming low power signals, a coupling and switching device comprising two identical resonant chambers, having their inputs coupled to said line at a common point through an iris opening in its outer conductor, and their outputs connected to said signal receiver through a T junction of individual output loops within the respective chambers, adjustable tuning means for each chamber and a discharge device connected across each chamber at a high impedance point, adapted to discharge to provide a low impedance shunt across the chamber effectively detuning it in response to a high resonant voltage such as would be applied by the high power signals entering the chamber through said iris opening and adapted to remain in the undischarged condition in response to the relatively lower resonant voltage which would be applied thereto by the low power signals entering the chamber through said iris opening, said individual output loops being relatively disposed so that they have radial symmetry about said T junction thus providing a ISO-degree phase difference in the outputs of the two chambers, the tuning means of one chamber being normally adjusted to make that chamber resonant to the frequency of said low and high power signals, the tuning means of the other chamber being normally adjusted so that the latter chamber is detuned from said frequency of said low and high power signals to provide a signal output equal and opposite to that of the detuned first chamber when the high power signals are applied to the inputs of the two cha-m* bers and substantially no output when low power signals are applied to the inputs of the two chambers at said common point, so that high power signal leakage through said one .chamber is substantially cancelled during signal transmitting intervals and the low power signals are transmit- 

